AU665139B2

AU665139B2 - Laser arrangements

Info

Publication number: AU665139B2
Application number: AU53834/94A
Authority: AU
Inventors: Graeme Lawrence Clark; Ewan Sutherland Livingstone
Original assignee: EEV Ltd
Current assignee: Teledyne UK Ltd
Priority date: 1993-01-20
Filing date: 1994-01-18
Publication date: 1995-12-14
Anticipated expiration: 2014-01-18
Also published as: DE4401611A1; GB9301085D0; FR2700897B1; GB2274541A; JPH06244480A; GB2274541B; US5450433A; AU5383494A; FR2700897A1

Description

i I/UU/U 1 2B/5/91 Regulation 3.2(2)

AUSTRALIA

Patents Act 1990

ORIGINAL

COMPLETE SPECIFICATION STANDARD PATENT Application Number: Lodged: 99 49 9 Invention Title: LASER ARRANGEMENTS 0 0 The following statement is a full description of this invention, including the best method of performing it known to us Lsr ~nepn~ SP/9106/GAS Laser Arrangements This invention relates to laser arrangements and more particularly, but not exclusively, to arrangements in which the laser active medium is a metal vapour such as, for example, copper vapour.

Laser apparatus generally requires that in addition to the material which is, or is to form, the laser active medium, a buffer gas or mixture of gases is also included within a discharge tube to enable sufficient gas pressure to be maintained for laser action to be possible. It has been found that the introduction of small quantities of hydrogen into a buffer gas, such as neon, may improve the operating efficiency of the laser in some cases, although the mechanism by which such an introduction facilities the laser action is not at present clearly understood. Other gases such a deuterium, nitrogen and oxygen may also give increased efficiency when added to a laser active medium and buffer gas. The quantities required for such efficiency enhancing gases to be effective are generally much smaller than the main buffer gas or gases, a typical arrangement having partial pressure of one hundred times less than the main buffer gas pressure.

The present invention arose from a consideration of the use of hydrogen or other Y efficiency improving gases in laser arrangements.

According to the invention there is provided a laser arrangement comprising a laser envelope containing material which in use forms at least part of a laser active medium; a main buffer gas or mixture of gases; and reservoir means located within the laser envelope IIPO 2 P/9106/GAS for delivering hydrogen, or some other gas the presence of which improvers laser efficiency, into the laser active medium and main buffer gas at a partial pressure dependent on the temperature of the reservoir means, which temperature is substantially solely determined by heating occurring within the envelope arising from the operation of the laser arrangement.

The efficiency improving gas may also constitute part of the buffer gas when released into the laser active medium but this is distinct from the "main" buffer gas or gases without which laser radiation could not be generated under normal operating conditions.

By employing the invention, heating of the reservoir is provided by the normal process taking place within the arrangement to obtain laser radiation, for example, it may be achieved by electrical discharges established within the laser envelope. The temperature is substantially solely determined by this as no separate provision is made for heating the reservoir means. There is no requirement therefore to include complicated heating circuits to supply current to resistor elements at particular times in relation to the laser operating cycle. Use of the invention enables heating of the reservoir means to its optimum temperature to be achieved automatically during operation of the laser arrangement, reducing the likelihood of malfunctions. The temperature of the reservoir means is determined by the geometry of the laser arrangement and the temperature required within the laser active medium to achieve the generation of laser radiation under steady state operating conditions. 'The temperature distribution throughout the arrangement may therefore be calculated and hence the optimum position or positions for the reservoir r ~U i' b ICL~ r t il~i~ 3 P/9106/GAS means.

The location of the reservoir means, and hence the temperature which it reaches during normal operation of the laser arrangement, enables the amount of hydrogen or other gas released into the envelope to be controlled to reach an optimum partial pressure at which dynamic equilibrium is established. For example, in a copper vapour laser arrangement, the laser active medium is maintained at a temperature in the region of 1500'C and is surrounded by insulating layers of material to give a temperature at the outer surface of the arrangement of the order of 200'C. Where it is wished to use hydrogen to improve laser efficiency, this can be supplied using a reservoir containing titanium hydride. The optimum partial pressure of hydrogen within the laser active medium is achieved when the reservoir is heated to approximately 600'C. As the !temperature gradient across the radius of the laser arrangement may be calculated, the reservoir or reservoirs containing the titanium hydride may be located at a desired radius to produce a particular volume of hydrogen evolved from the reservoirs.

By suitably locating the reservoir means, it is possible therefore to accurately release the required amount of hydrogen or other gas into the laser active medium without complex monitoring equipment. Also, as the reservoir means is located within the envelope, the whole structure may be made robust as the reservoirs can be located within o the normal envelope configuration and do not require, for example, side arms to house them. There is no need to permit external access to the reservoir means for example, for the supply of heating current.

C~ 4 IC-~ IP IP aL 4 i 4 P/9106/GAS When the laser arrangement ceases operation, temperatures within the envelope drop. As the reservoir temperature also decreases, hydrogen, or other efficiency enhancing gas, within the tube is collected by the reservoir means as it combines with the remaining reservoir material. Thus, relatively small amounts of a hydride, say, may be used to give long operating life times before replenishment is required.

The invention is particularly advantageously applied where the laser active medium is a metal vapour but it may also be used for other types of laser.

Preferably, the reservoir means comprises a plurality of reservoirs, These may be symmetrically located around the longitudinal axis of the laser arrangement and advantageously are spatially disposed on a circle in a plane transverse to the longitudinal axis. In one particular embodiment of the invention, the reservoirs are located on two concentric circles and in the same plane transverse to the longitudinal axis, to give a particularly compact Jistribution of reservoirs.

The reservoir means may consist of apertures within a normally provided component of the laser arrangement within which a reservoir material, such as a hydride or a deuteride, is located. However, advantageously, the reservoir means comprises a container within which material which dispenses hydrogen or said some other gas is contained. This may be, for example, a thin walled palladium vessel through which gas molecules may pass, dynamic equilibrium thus being substantially unaffected by its presence. Containers permit easy handling of the reservoirs when assembling or servicing the laser arrangement.

4 P/9106/GAS When the laser arrangement ceases operation, temperatures within the envelope drop. As the reservoir temperature also decreases, hydrogen, or other efficiency enhancing gas, within the tube is collected by the reservoir means as it combines with the remaining reservoir material. Thus, relatively small amounts of a hydride, say, may be used to give long operating life times before replenishment is required.

Preferably, the reservoir means comprises a plurality of reservoirs, These may be symmetrically located around the longitudinal axis of the laser arrangement and advantageously are spatially disposed on a circle in a plane transverse to the longitudinal axis. In one particular embodiment of the invention, the reservoirs are located on two concentric circles and in the same plane transverse to the longitudinal axis, to give a particularly compact distribution of reservoirs.

The reservoir means may consist of apertures within a normally provided component of the laser arrangement within which a reservoir material, such as a hydride or a deuteride, is located. However, advantageously, the reservoir means comprises a container within which material which dispenses hydrogen or said some other gas is contained. This may be, for example, a thin walled palladium vessel through which gas molecules may pass, dynamic equilibrium thus being substantially unaffected by its presence, Containers permit easy handling of the reservoirs when assembling or servicing the laser arrangement.

i t( i it P/9106/GAS In one particularly advantageous embodiment of the invention, the reservoir means is located between electrodes within the laser envelope between which, during use, an electrical discharge is established. Thus, the reservoir may be made accessible to the laser active medium for the evolved gas or gases along only a short pathway.

Advantageously, the laser envelope is sealed off such that there is no flow through of buffer gas during use. A laser arrangement in accordance with the invention is well suited to a sealed off mode of operation as once the reservoir material is located within the envelope there is no need for replenishment during normal operational use.

Preferably, a buffer gas or mixture of gases comprises a noble gas or gases such as neon, helium and argon. Advantageously, the buffer gas has a partial pressure within the range of 5 torr to 1 atmosphere and the hydrogen or said some other gas has a partial pressure in the range of 0.1 to 10 torr.

One way in which the invention may be performed is now described by way of example with reference to the accompanying drawings, in which: Figure 1 is a schematic longitudinal section through a metal vapour laser arrangement; and Figure 2 is a transverse section along the line II-II shown on Figure 1.

With reference to Figures 1 and 2, a copper vapour laser arrangement in I T l~ It~L~ll ~C1 e-rr i i 6 P/9106/GAS accordance with the invention has a substantially cylindrical configuration and includes an Sj outer glass vacuum envelope 1 coaxially arranged about the longitudinal axis X-X and i surrounding an alumina tube 2. Thermally insulating material 3 is positioned between the i envelope 1 and tube 2 and comprises a compacted alumina substance. End windows 4 and are located on the axis X-X which is also the optical axis along which laser radiation is Sgenerated during use. The arrangement firther includes two electrodes 6 and 7 at each i end of the alumina tube 2 and between which, in operation, a discharge is established to i provide pumping and excitation energy to the laser active medium. Each of the electrodes 6 and 7 is connected to metal end pieces 8 and 9 respectively by which electrical connection is made to the electrodes. The active laser medium in this case is copper vapour. Prior to use, therefore, copper 10, in the form of powder or metallic pieces, is distributed along the interior of the alumina tube 2.

A plurality of cylindrical apertures 11 is formed in the insulating material 3 at its end faces adjacent the metal end pieces 8 and 9, the apertures 11 being symmetrically arranged about the axis X-X. Figure 2 illustrates the group of apertures 11 at the left hand end as shown, those at the right hand end being arranged in a similar pattern. The apertures are extensive in a parallel direction to the axis X-X and are arranged on two concentric circles being equidistant and those on the inner circle being staggered with respect to those on the outer circle. Each aperture has a diameter of approximately 2mm and contains a palladium walled container 12 which, in this embodiment of the invention, contains powdered titanium hydride. Gaps between the end faces of the insulating material 3 and metal end pieces 8 and 9 permit a path for gas atoms and molecules to travel between the containers 12 and the interior of the alumina tube 2. In an alternative I ,F--CLI -1 7 P/9106/GAS embodiment (not shown) there are no gaps between the insulating material and end pieces, the gas diffusing from the containers 12 through the surrounding insulation to the laser amplification volume.

The laser envelope 1 contains neon buffer gas at a pressure of 10 Torr. The envelope 1 is sealed such that there is no flow of buffer gas through it under operating conditions.

During operation of the arrangement, repeated electrical discharges between the electrodes 6 and 7 cause the interior of the arrangement to become heated to a temperature of approximately 1500 0 C. At these temperatures the copper metal 10 vaporises and is excited to obtain a population inversion and hence generate laser radiation.

As the interior temperature of the laser arrangement rises on commencement, the thickness and thermal conduction properties of the insulating material 3 creates a temperature gradient in a radial direction, such that the outer surface of the vacuum S envelope reaches and remains at a temperature of approximately 200 0 C. The temperature at the two radii at which the containers 12 are located also gradually increases until after approximately ten minutes or so, they reach a steady state temperature of about 600'C. As the temperature of the titanium hydride increases, hydrogen is evolved which passes through the gaps between the insulating material 3 and end pieces 8 and 9 into the laser amplification volume. The partial pressure of the hydrogen increases as the temperature of the reservoir material rises until eventually a steady state pressure is attained when the final temperature of 600 0 C is reached. At this temperature, the partial pressure of 4 c ri eY~ ~LCICI ~1 pp..

8 P/9106/GAS hydrogen in the active laser volume is approximately 0.5 torr. The hydrogen contributes to the lasing mechanism and the operation of the laser arrangement to increase its operating efficiency.

When the laser arrangement is switched off, the interior defined by the glass envelope 1 slowly cools. As the titanium hydride in the containers 12 cools, it takes up hydrogen within the laser volume until gradually substantially all the hydrogen with the arrangement has returned to the reservoirs 12.

If it is wished to use deuterium as the efficiency enhancing element, a suitable material for use in the reservoirs is titanium deuteride.

Although the invention is described with reference to a copper vapour laser, it is equally applicable to gold or some other metal, or mixture of metal, vapours and to other types of laser. Similarly the reservoir material is chosen to evolve the desired efficiency enhancing gas. The placement of a reservoir or reservoirs is determined by the thermal gradients set up under operating conditions and the temperature at which the required amount of the gas is liberated.

The efficiency enhancing gas may be one, or a mixture of, hydrogen, deuterium, nitrogen and oxygen.

L~ Ir -C -rC t' I 'II

Claims

1. A laser arrangement comprising: a laser envelope containing material which in use forms at least part of a laser active medium; reservoir means; a main buffer gas or mixture of gases; and thermally insulating material located within the laser envelope, the reservoir means being located in the insulating material for delivering hydrogen, or some other gas the presence of which improves laser efficiency, into the laser active medium and main buffer gas at a partial pressure dependent on the temperature of the reservoir means, which temperature is substantially solely determined by heating occurring within the envelope arising from the operation of the arrangement, the location of the reservoir means on the temperature gradient across the insulating material defining the temperature of the reservoir means.

2. An arrangement as claimed in claim 1 wherein the laser active medium is a metal vapour.

3. An arrangement as claimed in claim 1 or 2 wherein the reservoir means comprises a plurality of reservoirs.

4. An arrangement as claimed in claim 3 wherein the reservoirs are spatially disposed on a circle in a plane transverse to the longitudinal axis of the arrangement.

An arrangement as claimed in claim 4 wherein the reservoirs are disposed on a plurality of coaxial circles arranged coaxially about one another and the longitudinal axis.

6. An arrangement as claimed in any preceding claim wherein the reservoir means comprises at least one container containing material which dispenses hydrogen or said (DOC 05 AU5383494.WPC SKP/PVF:KP) P/9106/GAS some other gas when the reservoir is heated.

7. An arrangement as claimed in any preceding claim wherein said reservoir means is located between electrodes within the laser envelope between which, during use, an electrical discharge is established.

8. An arrangement as claimed in any preceding claim wherein the laser envelope is sealed off such that there is io flow through of buffer gas during use.

9. An arrangement as claimed in any preceding claim wherein where the efficiency gas is hydrogen, the reservoir means includes a hydride material.

An arrangement as claimed in any of claims 1 to 8 wherein where said some other gas is deuterium, the reservoir means includes deuteride. 4

11. An arrangement as claimed in any preceding claim wherein the buffer gas or mixture of gases comprises a noble gas or gases.

12. An arrangement as claimed in any preceding claim wherein the buffer gas has a pressure within the range 5 torr to 1 atmosphere and the hydrogen or said some other gas has a pressure in the range of 0.1 to 10 torr.

13. A laser arrangement substantially as illustrated in and described with reference to the accompanying drawings. DATED this 18th day of January 1994. EEV LTD. WATERMARK PATENT TRADEMARK ATTORNEYS 290 BURWOOD ROAD, HAWTHORN. VIC. 3122. 1417 11 P/9106/GAS ABSTRACT Laser Arrangements A laser arrangement includes an outer envelope 1 and an inner alumina tube 2 between which insulating material 3 is located. The insulating material has a plurality of apertures 11 therein in its transverse end faces, the apertures being arranged at each end on two circles of similar radii. Hydrogen reservoirs 12 are located within the apertures 11. During operation of the laser arrangement, the reservoirs 12 become heated causing hydrogen to be evolved and diffused through to the laser active medium, improving the efficiency of the laser processes. When laser action ceases, the arrangement cools and hydrogen returns to the reservoirs 12. Other efficiency enhancing gases may be used in a the reservoirs. 1 e